US4405986A - GSP/Doppler sensor velocity derived attitude reference system - Google Patents
GSP/Doppler sensor velocity derived attitude reference system Download PDFInfo
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- US4405986A US4405986A US06/255,030 US25503081A US4405986A US 4405986 A US4405986 A US 4405986A US 25503081 A US25503081 A US 25503081A US 4405986 A US4405986 A US 4405986A
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
- G01S13/86—Combinations of radar systems with non-radar systems, e.g. sonar, direction finder
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
- G01S13/87—Combinations of radar systems, e.g. primary radar and secondary radar
- G01S13/874—Combination of several systems for attitude determination
Definitions
- This invention relates to an aircraft instrument, and more particularly to a novel attitude reference instrument which determines the aircraft's instantaneous pitch and roll angles from a plurality of measured aircraft velocities.
- Some of the velocities are obtained from a satellite navigation system, for example, the Global Positioning System, known as the GPS NAVSTAR, and other of the velocities are obtained from on-board velocity measuring equipment, for example a Doppler radar sensor, which may form a portion of a standard Doppler navigator, for example, the AN/ASN-128.
- the invention provides an attitude reference which is not directly dependent on the use of gyroscopes and thus obviates many of the disadvantages of these instruments.
- gyroscopes are subject to tumbling if the aircraft exceeds certain limits of pitch and/or roll, as well as precession and drift errors.
- the present invention can function as a redundant backup system for a conventional gyro type attitude reference and can also be used for dynamic calibration and alignment of such a gyro attitude reference.
- the aircraft is provided with an antenna atop its fuselage which conveys signals from a plurality of orbiting navigation satellites to a receiver/processor. Each satellite transmits a range signal and a range rate signal.
- the receiver/processor correlates the received signals with stored ephemeris information regarding the orbits of all the satellites and yields from this information three velocities, namely V n , V e , and V v . These are further correlated with the output of a heading reference, for example a directional gyro, to obtain two additional velocities, V h and V d , these being the along-track and cross-track velocities, respectively, in a plane tangent to the earth at the location of the aircraft.
- a heading reference for example a directional gyro
- the doppler sensor by means of well known techniques, radiates a plurality of radar beams toward the earth and determines the aircraft's ground speeds along its roll, pitch and yaw axes. These speeds are V x , V y , and V z respectively.
- the Doppler-derived velocities will undergo cyclic variations caused by the attitude changes, for example, if the aircraft cyclically pitches, the Doppler beams will undergo a corresponding back and forth motion which will modulate the velocity V x along the roll axis at the pitching rate and by an amount related to the amplitude of the pitching motion. This modulation due to pitching will be superimposed on the speed V x which would obtain in the absence of pitching, that is if the aircraft were flying straight and level in smooth air.
- V h , V d , and V v are true ground speeds which include the effects of all aircraft motion including pitching and rolling
- correlation or comparison of the satellite-derived velocities with the Doppler-derived velocities can yield pitch and roll information.
- This correlation or comparison takes place in a velocity processor to which the six velocities are applied. This circuit processes its inputs in accordance with an algorithm to be presented.
- strapped-down accelerometers may be used to measure aircraft acceleration along its three orthogonal axes, and their outputs integrated to obtain the three axial velocities, which are correlated with the along-track and cross-track velocities to obtain the desired pitch and roll information.
- Another object of the invention is to provide circuitry for determining the pitch and roll of an aircraft by utilizing a plurality of velocity measurements derived from two separate sources and heading information from a heading reference.
- a further object of the invention is to provide an indication of an aircraft's instantaneous pitch and roll which is not subject to gyro drift error or gyro tumbling and which can be used either as a primary attitude instrument or as a backup for conventional attitude indicators, or as a calibration standard therefor.
- FIG. 1 is a pictorial-block diagram of an illustrative embodiment of the invention.
- FIG. 2 is a vector diagram showing the relationship between the satellite-derived velocities and the along-track and cross-track velocities.
- FIGS. 3 and 4 are coordinate systems showing how the GPS-derived velocities are obtained and transformed from one coordinate system to another.
- FIG. 5 shows how the circuitry of FIG. 1 would be modified if accelerometers and integrators were used to obtain the three aircraft axial velocities.
- the GPS system is a satellite referenced radio navigation system consisting of 24 satellites orbiting in three different planes and spaced along their orbits such that four or more satellites are visible at all times at any place on earth.
- a ground tracking network periodically measures and updates the ephermeris of each satellite and keeps all satellite clocks synchronized.
- Each satellite continually transmits orthogonally binary coded ranging signals to users.
- the GPS user can measure the time delay of the transmitted signal. This time delay not only includes the signal propagation delay but also the clock bias and clock bias rate differences between the user's clock and the satellite clocks.
- the GPS user equipment comprising an antenna and a receiver/processor connected thereto, can be used to determine user position and velocity by measuring the GPS signal time of arrival together with GPS signal Doppler shift. This is done by receiving all available satellite signals from which four satellites are selected to establish four independent pseudo range and pseudo range rates. Since the user's clock bias, or error, is common to all range measurements, it induces a time error into these measurements which is directly related to the range error by a constant factor, namely the speed of light. Therefore, the clock bias, which is actually a phase difference using quartz clocks, can be treated as a bias error source in the range measurement. Thus the initially measured range is referred to as a pseudo range rather than a true range.
- the pseudo range measurement, P i is a scalar quantity equal to the biased magnitude of the vector difference between the user's position and the satellite position.
- P i the pseudo range measurement
- the present invention is intended for use with the GPS system or with its functional equivalent.
- the invention will be described in connection with the illustrative embodiment shown in FIG. 1.
- the aircraft 11 therein includes an antenna 21 atop its fuselage where it has an unobstructed view of four GPS orbiting satellites 13, 15, 17, and 19.
- the received GPS signals are applied by the antenna to GPS receiver/processor 23 where the north velocity V n , the east velocity V e , and the vertical velocity V v are derived therefrom, in a manner to be explained.
- a heading reference 36 which may be a conventional directional gyro, provides a continuous heading signal, H.
- the velocities V n , V e , and V v are applied to converter 26, together with the heading signal H.
- the converter 26 calculates from these inputs two additional velocities, namely V h and V d , these being the along-track and cross-track velocities of the aircraft, respectively.
- the vector diagram of FIG. 2 shows the relationships between these velocities.
- V n is the velocity of the aircraft along the local meridian and V e is its velocity along the local parallel of latitude.
- FIG. 2 shows the aircraft 11 at the origin of the coordinate system with velocity V h along its heading and drift or cross-track velocity of V d at a 90° angle thereto.
- the heading angle H is that between true north and V h . All of these velocities are in a plane parallel to the earth at the position of the aircraft.
- FIG. 4 illustrates such a plane tangent to a sector of the earth. Since the north velocity must be equal to the northerly component of the vector sum of V h and V d , the following equation can be written,
- the east velocity V e must be equal to the easterly component of the vector sum of V h and V d , thus,
- the circuit of converter 26 of FIG. 1 is designed to calculate these two velocities by carrying out the operations indicated by equations (3) and (4).
- the vertical velocity V v also appears at the output of converter 26. It is merely passed through this circuit.
- the aircraft includes on its underside a Doppler antenna array 29 adapted to radiate four beams of microwave energy 1, 2, 3, and 4 toward the earth 32, and receive backscattered energy therefrom.
- the Doppler receiver/processor 31 receives the backscattered echo signals, correlates them with a sample of the transmitted signal to obtain the Doppler signals indictive of the aircraft's velocity along its three orthogonal axis, V x , V y , and V z .
- These axial velocities are those along the roll, pitch and yaw axes, respectively.
- the velocities V x and V y are not necessarily parallel to or tangent to the earth, unless the aircraft is flying straight and level in smooth air.
- thes axial velocities are constantly changing in direction due to pitching and rolling of the aircraft.
- these axial velocities would be correlated with pitch and roll information obtained from a vertical gyro or the like, to obtain the along-track and cross-track velocities.
- correlation between V h , V d , and V x , V y , and V z should yield the pitch and roll information usually obtained from a vertical gyro.
- This correlation or calculation is performed by velocity processor 24 which solves an equation or algorithm to be derived below to obtain the instantaneous pitch and roll angles of the aircraft. These angles are applied to attitude readout 28 which can be mounted on the aircraft's panel for the benefit of the crew and also used for the other purposes discussed above.
- the global diagram of FIG. 3 illustrates how the GPS receiver circuitry calculates the GPS velocities.
- the diagram is a Cartesian Earth-centered reference (ECR) coordinate system with the origin, O, of the mutually orthogonal X, Y and Z axes at the center of the earth.
- the vehicle 11 with the present invention aboard is shown at coordinates X, Y and Z, with the i th , satellite at coordinates U i , V i and W i .
- the symbol r represents the radius of the earth which passes through the vehicle 11 and P the range of the i th satellite.
- the position fixing equation for the vehicle 11 is: ##EQU1## wherein; P i equals the measured pseudo range, B is the satellite to user clock bias.
- P i equals the measured pseudo range
- B is the satellite to user clock bias.
- This pseudo range rate is the biased magnitude of the vector difference, along the line of sight, between the user's velocity and the satellite velocity.
- the GPS velocity fixing equations are: ##EQU2## wherein, X, Y and Z are the vehicle velocities, P i is the measured pseudo range rate and U, V and W, are the satellite velocities along the three coordinate axes, obtained from the orbital data stored in memory, B is the satellite to user clock bias rate or frequency bias, and, ##EQU3## Thus RHO i is the positional information obtained in the preceding step.
- Four simultaneous equations like Eq. (6) can be written for each of the four satellites and can be solved to yield all four unknowns. The results are the vehicle velocities along the X, Y and Z axes of FIG. 3.
- FIG. 4 illustrates how this transformation is made.
- 49 represents a sector of the earth, with r the earth's radius and the X, Y and Z coordinate system of FIG. 3 drawn thereon.
- Point O indicates the earth's center and the plane 51 represents a plane tangent to the earth at the location of the vehicle 11.
- the local meridian 52 is shown.
- the angle of latitude L of the vehicle is the angle which radius r makes with the equator 54, measured along the local meridian 52.
- the angle M between the X axis and the local meridian is the longitude.
- the previously derived velocities V x , V y and V z are shown, together with the required transformation thereof, V n and V e .
- V v is the radial component of velocity along an extension of the earth's radius r.
- the vehicle velocities, V x , V y and V z are the same velocities indicated by the symbols X, Y and Z in Eq. (6).
- r (X 2 +Y 2 +Z 2 ) ⁇ 5 .
- a Doppler navigator utilizes this relationship to derive the along-track and cross-track velocities from the axial velocities and pitch and roll information.
- the derivation of this matrix is discussed in detail in the aforementioned co-pending application of the present inventor.
- velocity processor 24 The algorithm or formula used by velocity processor 24 is determined as follows:
- equation (11) The first two equations from the above matrix, equation (11), are as follows,
- the roll of the aircraft can be obtained from equation (13), rearranged as follows,
- Equation (18) is now in quadratic form and can be solved for its roots, sin R, as follows, ##EQU6## Therefore the angle of roll is the arcsine of the right side of equation (19).
- equation (19) yields two roots and thus two roll angles. Obviously only one of these angles is the correct one, and it can be selected by initializing the system to a known roll condition, for example, to zero roll with the aircraft on level ground or flying straight and level, and comparing the two derived roll angles to the initial condition.
- the velocity processor 24 can be programmed to automatically perform this function.
- the velocity processor 24 is adapted to determine the instantaneous pitch and roll angles by utilizing equations (24) and (19), and provides a continuous indication of these two angles to readout 28.
- FIG. 5 shows what the aircraft circuitry would be if the aforementioned strapped-down accelerometers were used to obtain the three axial velocities, in place of the Doppler radar equipment of FIG. 1.
- three accelerometers in circuit 45 are attached to the aircraft 11 in such a way that they sense mutually orthogonal accelerations along the roll, pitch and yaw (or X, Y, and Z) axes of the aircraft.
- the outputs of these accelerometers are applied to integrator 47 which mathematically integrates these signals to yield the axial velocities, V x , V y , and V z .
- These velocities are then applied to velocity processor 24, which is the same circuit as in FIG. 1, and which functions in the same way to calculate the desired attitude information.
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Abstract
Description
V.sub.n =V.sub.h cos -V.sub.d sin H Eq. (1)
V.sub.e =V.sub.d cos H+V.sub.h sin H Eq. (2)
V.sub.h =V.sub.n cos H+V.sub.e sin H Eq. (3)
V.sub.d =V.sub.e cos H-V.sub.n sin H Eq. (4)
X=V.sub.x =-V.sub.n sin L cos M+V.sub.v cos L cos M-V.sub.e sin M Eq. (8)
Y=V.sub.y =V.sub.v cos L sin M+V.sub.e cos M-V.sub.n sin L sin M Eq. (9)
Z=V.sub.z =V.sub.v sin L+V.sub.n cos L Eq. (10)
V.sub.h =V.sub.x cos PH+V.sub.y sin PH sin R+V.sub.z sin PH cos R Eq. (12)
V.sub.d =V.sub.y cos R-V.sub.z sin R Eq. (13)
V.sub.d +V.sub.z sin R=V.sub.y cos R Eq. (14)
V.sub.d.sup.2 +2V.sub.d V.sub.z sin R+V.sub.z.sup.2 sin.sup.2 R=V.sub.y.sup.2 cos.sup.2 R Eq. (15)
V.sub.d.sup.2 +2V.sub.d V.sub.z sin R+V.sub.z.sup.2 sin.sup.2 R=V.sub.y.sup.2 (1- sin.sup.2 R) Eq. (16)
[V.sub.d.sup.2 -V.sub.y.sup.2 ]+(V.sub.z.sup.2 +V.sub.y.sup.2) sin.sup.2 R+2V.sub.d V.sub.z sin R=0 Eq. (17)
V.sub.h =V.sub.x cos PH+V.sub.y sin PH sin R+V.sub.z sin PH cos R Eq. (20)
-V.sub.v =-V.sub.x sin PH+V.sub.y cos PH sin R+V.sub.z cos PH cos R Eq. (21)
V.sub.h =V.sub.x cos PH+[V.sub.y sin R+V.sub.z cos R]·sin PH Eq. (22)
-V.sub.v =-V.sub.x sin PH+[V.sub.y sin R+V.sub.z cos R]·cos PH Eq. (23)
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US06/255,030 US4405986A (en) | 1981-04-17 | 1981-04-17 | GSP/Doppler sensor velocity derived attitude reference system |
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US5406489A (en) * | 1992-07-10 | 1995-04-11 | Unisys Corporation | Instrument for measuring an aircraft's roll, pitch, and heading by matching position changes along two sets of axes |
US5477458A (en) * | 1994-01-03 | 1995-12-19 | Trimble Navigation Limited | Network for carrier phase differential GPS corrections |
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US5805200A (en) * | 1982-03-01 | 1998-09-08 | Western Atlas International, Inc. | System for determining position from pseudorandomly modulated radio signals |
US5014066A (en) * | 1982-03-01 | 1991-05-07 | Western Atlas International, Inc. | System for simultaneously deriving position information from a plurality of satellite transmissions |
US5619212A (en) * | 1982-03-01 | 1997-04-08 | Western Atlas International, Inc. | System for determining position from suppressed carrier radio waves |
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EP0322349A2 (en) * | 1987-12-23 | 1989-06-28 | Hughes Aircraft Company | Satellite attitude determination and control system with agile beam sensing |
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US5406489A (en) * | 1992-07-10 | 1995-04-11 | Unisys Corporation | Instrument for measuring an aircraft's roll, pitch, and heading by matching position changes along two sets of axes |
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